Exotic Stars: Extreme Physics Flashcards

1
Q

How do exotic stars form?

A

Nuclear fuel runs out
Thermal pressure fails
Gravitational collapse to smaller size
New equilibrium between gravity and quantum degeneracy pressure

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2
Q

What kind of stars are exotic?

A

White dwarf stars

Neutron stars

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3
Q

Why are exotic stars useful?

A

Strong tests of quantum mechanics, special and general relativity

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4
Q

Type 1a supernova

A

When a white dwarf has a companion and explodes

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5
Q

How much energy is released in a type 1a supernova

A

Suns lifelong output

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6
Q

How hot is a type 1a supernova

A

100 Tsun

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7
Q

How bright is a type 1a supernova

A

5 billion x Lsun (about a galaxy)

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8
Q

Mysteries of the type 1a supernova

A

Single/double degenerate progenitors

How does the explosion happen in detail

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9
Q

Type 1a supernovae - recent supercomputer simulations

A

Ignition not from gravitational collapse?
Pressure and temp slowly increase until Tcore reaches fusion temp right before M reaches Mch
Small flame bubble starts near centre
OR
Nuclear burn (flame starts from carbon fusion,oxygen fusion stars later, subsonic deflagration -> supersonic detonation)

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10
Q

Type II supernova

A

Stars mass > 8-10 sun
Onion layered fusion with Inert nickel iron core (WD) supported by electron degeneracy pressure
Nickel iron ash deposited until core mass reaches Mch and collapses
Electrons squish until they fuse with protons to make neutrons
Outer shell free falls in

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11
Q

Type II supernova what is the collapse halted by? What happens after?

A

Repulsive strong force and neutron degeneracy
There’s a bounce
Them an outward moving shockwaves
Only sun’s lifetime output involved in visible blast which leaves behind rest

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12
Q

Mysteries of Type II supernova

A

Nature of short range nuclear forces
How burst of neutrinos converts 1% of energy to produce shock wave that causes SN explosion
Hypernovae, gamma ray bursts etc

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13
Q

What are neutron stars?

A

Giant atomic nucleus
Strong gravitational field
Strong magnetic field
Rapid rotation - pulsar

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14
Q

How do you get from white dwarf to neutron star

A

me -> mn ~ mp

Mu=2 -> mu=1

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15
Q

Chandrasekhar limit

A

1) Emax = cp
2) p max = cNe^1/3h/2R
3) Pmax = NkT/V = N/V (2Emax/3)
4) Pc = Pmax

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16
Q

Inert white dwarf

A

Core held up by electron degeneracy pressure
H burning she’ll deposits ash, growing core
Wind from burning expels outer layers - red giant - planetary nebula
Wind is fast enough that M doesn’t exceed Mch

17
Q

White dwarf supernova

A
WD core orbiting companion star
H pulled onto WD by tidal forces
M slowly increases until M=Mch
Supernova 
Nuclei free fall until gravity
Temp up
Flash nuclear burn
18
Q

Death of a high mass star

A

1) more massive core - hotter core

2) loss of mass during giant phase can’t keep mass less than Mch

19
Q

Parts of a supernova

A

Collapse
Bounce
Explosion

20
Q

Supernova - collapse

A

Core - gas of e and Fe, v->c
Gravitational collapse
Beta decay happens (n formed)

21
Q

Supernova - bounce

A

Repulsive nuclear force at short distance

Neutron degeneracy pressure

22
Q

Supernova - explosion

A

Energy of stellar mass is only 10^44J

Neutrinos carry away almost all the 10^46J of gravitational PE

23
Q

Neutron stars

A

All nuclei have same density
Strong nuclear force has hard core of repulsion (not understood)
Stabilized by gravity (against repulsive force)

24
Q

Neutron stars - strong gravitational field

A

Can use Newtonian gravity as rough approx

25
Q

Neutron stars - strong magnetic field

A

Plasma is highly conducting
B lines frozen into plasma
Plasma in tube of B lines always remains as plasma moves
In NS same number of B lines through tiny area
Charged particles spiral around them
-photons split in two
-vacuum itself is polarized

26
Q

Neutron stars - rapid rotation

A

Conservation of angular momentum
Changing B field is changing E field
Pulsars lol